diff --git "a/D9E0T4oBgHgl3EQfggHn/content/tmp_files/load_file.txt" "b/D9E0T4oBgHgl3EQfggHn/content/tmp_files/load_file.txt" new file mode 100644--- /dev/null +++ "b/D9E0T4oBgHgl3EQfggHn/content/tmp_files/load_file.txt" @@ -0,0 +1,1918 @@ +filepath=/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf,len=1917 +page_content='Noname manuscript No.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' (will be inserted by the editor) The shape of gold B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Bally1,2,a, G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Giacalone3,b, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Bender4,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='c 1 ESNT,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' IRFU,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' CEA,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Universit´e Paris-Saclay,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 91191 Gif-sur-Yvette,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' France 2 Departamento de F´ısica Te´orica,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Universidad Aut´onoma de Madrid,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' E-28049 Madrid,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Spain 3 Institut f¨ur Theoretische Physik,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Universit¨at Heidelberg,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Philosophenweg 16,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' D-69120 Heidelberg,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Germany 4 Universit´e de Lyon,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Universit´e Claude Bernard Lyon 1,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' CNRS/IN2P3,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' IP2I Lyon,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' UMR 5822,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 4 rue Enrico Fermi,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' F-69622,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Villeurbanne,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' France Received: January 9,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 2023 / Revised version: date Abstract Having a detailed theoretical knowledge of the low-energy structure of the heavy odd-mass nucleus 197Au is of prime interest as the structure of this isotope represents an important input to theoretical simulations of collider experiments involving gold ions performed worldwide at relativistic energies.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' In the present article, therefore, we report on new results on the structure of 197Au obtained from state-of-the-art multi-reference energy density functional (MR-EDF) calculations.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Our MR-EDF calculations were realized using the Skyrme- type pseudo-potential SLyMR1, and include beyond mean-��eld correlations through the mixing, in the spirit of the Generator Coordinate Method (GCM), of particle- number and angular-momentum projected triaxially de- formed Bogoliubov quasi-particle states.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Comparison with experimental data shows that the model gives a reasonable description of 197Au with in particular a good agreement for most of the spectroscopic proper- ties of the 3/2+ 1 ground state.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' From the collective wave function of the correlated state, we compute an average deformation ¯β(3/2+ 1 ) = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='13 and ¯γ(3/2+ 1 ) = 40◦ for the ground state.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' We use this result to construct an intrinsic shape of 197Au representing a microscopically-motivated input for precision simulations of the associated collider processes.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' We discuss, in particular, how the triaxial- ity of this nucleus is expected to impact 197Au+197Au collision experiments at ultrarelativistic energy.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 1 Introduction For millennia, gold has held a prominent role in human societies, whether it be as a symbol of wealth, a stan- aE-mail: benjamin.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='bally@cea.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='fr bE-mail: giacalone@thphys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='uni-heidelberg.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='de cE-mail: bender@ip2i.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='in2p3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='fr dard in international economic trades or because of its medicinal and industrial applications.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Interestingly, all the gold of the world, whether it is used as jewelry, in computer chips or kept in secured bank vaults, shares one important feature: it is made of a single isotope.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Indeed, zooming in on the structure of this special el- ement at the nuclear scale, one discovers that there is only one stable gold isotope known to exist, namely 197Au.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' As a matter of fact, nuclear physics essentially began with the 197Au nucleus, which has been the first to be discovered in 1909 by Rutherford, Geiger and Mardsen from the scattering of α particles off a gold foil [1,2].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Over 100 years later, we have now a wealth of data available on the structure of 197Au [3–10].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' The low-energy spec- trum of the nucleus is well known and electromagnetic moments were measured for the ground state as well as for several excited states [11,12].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Within a simple single- particle picture, the 3/2+ 1 ground state of 197Au can be interpreted as a proton 2d3/2 particle (hole) coupled to a 196Pt (198Hg) core.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Considering the naive picture of a many-body state built as the product of independent harmonic oscillator single-particles (holes) on top of a suitably chosen core, oblate deformations are favoured for nuclei close to the end of a major shell [13,14].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Given the proximity of the Z = 82 and N = 126 shell closures, we can thus expect 197Au to adopt a small oblate-like deformation.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Actually, axially-symmetric mean-field cal- culations based on the Gogny D1S functional [15, 16] reported in the AMEDEE database [17] do find an oblate minimum with a magnitude of β ≈ 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='12.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Starting from the early 2000’s, 197Au has played a cen- tral role as well in high-energy nuclear physics.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Indeed, gold ions are employed in various scattering experiments ranging from fixed-target experiments at a nucleon- arXiv:2301.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='02420v1 [nucl-th] 6 Jan 2023 2 nucleon center-of-mass energy of 2-3 GeV performed at GSI, Darmstadt, to ultrarelativsitic collisions at a nucleon-nucleon center-of-mass energy of 200 GeV per- formed at the at the BNL Relativsitic Heavy Ion Collider (RHIC).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Gold is, in particular, the prime species used at the BNL RHIC, and the first conclusive evidence of the formation of quark-gluon plasma in a laboratory has been indeed obtained in ultrarelativistic 197Au+197Au collisions [18–21].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' The theoretical interpretation of the results of high- energy scattering experiments starts with an input from nuclear structure theory [22].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' The great success of the hydrodynamic modeling of the quark-gluon plasma [23] combined with the availability of data from collisions of several ion species has recently lead to a precise identifi- cation of the impact of the structural properties of the collided nuclei on several experimental observables.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' In particular, the azimuthal distributions of particles pro- duced in relativistic collision experiments are observed to present a strong sensitivity to spatial correlations of nucleons (i.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' deformations) in the ground-state many- body wave function of the colliding species [24–29].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' For example, in a recent article [30], we argued that we could identify fingerprints of the triaxiality of 129Xe in collisions performed at the CERN Large Hadron Collider (LHC).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' The picture of a triaxial 129Xe drawn from the analysis of high-energy data [31] is in excel- lent agreement with results obtained from low-energy Coulomb excitation experiments performed on the ad- jacent isotopes, 128,130Xe [32, 33], as well as with our recent theoretical calculations dedicated to these three xenon isotopes [34].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Our goal for this manuscript is, in a sense, to perform a similar analysis focused on 197Au, to assess and potentially improve the current structure input to high-energy 197Au+197Au collisions.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' To this aim, we first investigate the low-energy structure of 197Au on microscopic grounds using the MR-EDF formalism [35,36].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' More precisely, we present new results obtained from state-of-the-art calculations based on the configuration mixing of symmetry-projected triaxially deformed Bogoliubov quasi-particle states [37–42] and the use of the Skyrme-type pseudo-potential SLyMR1 [43,44].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Secondly, we employ these results to construct a point-nucleon density for 197Au, which we subsequently employ in state-of-the-art simulations of the initial states of high-energy 197Au+197Au collisions.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' We point out, thus, the expected consequences of implementing our newly-derived nucleon density in future hydrodynamic simulations of such processes, with a focus on the role played by the presence of a slight triaxiality in the colliding ions.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' This article is organized as follows: In Sec.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 2, we re- port on MR-EDF calculations dedicated to the study of the structure of 197Au.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Then, in Sec.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 3 we analyze the consequences of our results on the modeling and the ob- servables of relativistic heavy-ion collisions.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Finally, our conclusions and prospects are reported in Sec.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 2 Nuclear structure 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1 Method In the present study, we use the same theoretical frame- work as the one that was presented in Ref.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' [34] and refer to that article for more details on our method such as the definitions of the usual operators or the symmetries used in our calculations.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Nevertheless, to deal with the heavy-mass 197Au nucleus we changed a few numerical parameters compared to the ones used in Ref.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' [34].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Firstly, the Bogoliubov reference states were represented on a three-dimensional Cartesian La- grange mesh [45] in a box of 32 points in each direction.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Secondly, when exploring the triaxial deformations, we used a mesh with a spacing1 ∆q1 = ∆q2 = 375 fm2 starting from (q1, q2) = (0, 0) and restricting ourselves to positive values of q1 and q2, which maps the first sextant of the β-γ plane.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Finally,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' concerning the cutoffs applied during the mixing of reference states: before the mixing,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' we remove the projected components that in the decomposition of the original reference states have a weight that is lower than 10−3,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' whereas during the mixing of K-components (performed individually for each reference state) we remove the norm eigenstates with an eigenvalue smaller than 10−2,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' and during the final diagonalization mixing projected states originating from different Bogoliubov vacua,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' we remove the norm eigenstates with an eigenvalue smaller than 10−4 for all nuclei.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' The values for the the cutoffs are more restric- tive than the ones used when tackling the 128,129,130Xe isotopes because the configuration mixing performed in the present calculations for 197Au proved to be more sensitive to the inclusion of components with a small weight that are probably not well represented on our cartesian mesh and, therefore, have to be discarded.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Un- fortunately, the improvement of the numerical accuracy of our lattice, by increasing the number of mesh points and/or reducing the spacing between them, implies a substantial increase of the computational cost of the MR-EDF calculations that is at present out of reach for us.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 1When considering axial deformations, this corresponds to a step of ∆β ≈ 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='05.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 3 Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 1: Particle-number restored total energy surfaces for 197Au and π = +1 (top panel) or π = −1 (bottom panel).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Black lines are separated by 1 MeV.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' The minimum for positive (negative) parity, indicated by a silver star, is located at a deformation of β = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='12 and γ = 38◦ (β = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='12 and γ = 19◦) 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='2 Structure of 197Au 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1 Energy surfaces The first step in our approach is the generation of a set of one-quasi-particle states that will be used as reference states in the final configuration mixing calculations.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' To generate and select the reference states, we follow the strategy detailed in Ref.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' [34].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' We briefly recall here that this implies: i) the self-consistent blocking of four different one-quasi-particle states at each point of the deformation mesh, ii) the projection onto good particle numbers and good angular momentum of all (converged) one-quasi-particle states, and iii) the selection of the ones having a projected energy lower than a given threshold above the projected minimum of same parity.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' In this work, we use a threshold of 5 MeV for both positive and negative parity states.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' But before discussing the final results obtained after con- figuration mixing, let us first analyze the intermediate steps in our method.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Figure 1 displays the particle- number restored (PNR) total energy surface for the positive and negative parity states of 197Au.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' As can be seen, the two energy surfaces exhibit a γ-soft topography with a slightly deformed minimum2 located at β = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='12.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Also, we notice that the surface for positive parity is softer at small deformation than the surface for negative parity.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Finally, the minimum for positive parity states is approximately 200 keV lower than the one for negative parity states.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Performing the full symmetry restoration, we display in Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 2 the angular-momentum and particle-number restored (AMPNR) total energy surfaces for the lowest Jπ = 1/2+, 3/2+ and 11/2− projected states, which are the three values of Jπ giving the lowest projected energies.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' A first remark is that the energy surfaces are much more rigid with now a well pronounced triaxial minimum with β = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='13.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Compared to the PNR case, the minima of the AMPNR surfaces gain rouhgly 5 MeV in binding energy and the absolute minimum is obtained for Jπ = 3/2+.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' It is also worth mentioning that the one- quasi-particle state giving the lowest projected state is obtained by blocking a quasi-particle that is dominated by a single-particle state originating from the spherical 2d3/2 shell.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' The latter observations are consistent with the experimental spin-parity assignment 3/2+ 1 for the ground state of 197Au as well as its naive single-particle interpretation.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' However, we notice that the minimum for the Jπ = 3/2+ surface is located at a deformation with an angle γ = 24◦, which seems to be at variance with the oblate-like shape expected from simple argu- ments as mentioned above.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Nevertheless, it is important to remark that the configuration mixing may change this picture.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' In addition, we displayed in Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 2 only the surface for the lowest Jπ = 3/2+ projected states, but given the fact that we explore triaxial deformations, all the reference states with a non-zero average value of γ will generate after angular-momentum restoration two projected states with Jπ = 3/2+ that will enter the configuration mixing.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Ultimately, given the fact that the AMPNR is only an intermediate step in our approach, it is neither possible nor desirable to definitively charac- terize the structure of the final correlated state at this level of approximation.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Additionally, we note that the angular-momentum pro- jection does not shift the energy minimum towards larger values of β compared to the plain PNR case, which is 2Note that all the extrema discussed in this article are com- puted from an interpolation based on the results obtained at the points on the discretized deformation mesh.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 4 Jπ = 1/2+ Jπ = 3/2+ Jπ = 11/2− Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 2: Angular-momentum and particle-number re- stored total energy surface for 197Au and for the lowest Jπ = 1/2+ (top panel), the lowest Jπ = 3/2+ (mid- dle panel) and lowest Jπ = 11/2− (bottom panel).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Black lines are separated by 1 MeV.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' The minima for Jπ = 1/2+, 3/2+ and 11/2−, indicated by silver stars, are located at deformations of β = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='13 and γ = 39◦, β = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='13 and γ = 24◦ and β = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='13 and γ = 22◦, respectively contrary to what is often observed in MR-EDF calcula- tions [30,37–40].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 3: Low-energy spectrum for 197Au.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Experimental data are taken from [46], which are based on the evalu- ation [3] 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='2 Low-energy spectroscopy Finally, we perform the full configuration mixing of sym- metry projected reference states considering for positive (negative) parity a set containing 24 (19) one-quasi- particle states.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' In Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 3 we compare the theoretical results to the available experimental data for the low- lying states up to 1 MeV of excitation energies.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' First of all, we remark that the theory is able to reproduce the spin-parity assignment for the ground state (3/2+ 1 ) as well as for the the first (1/2+ 1 ), second (3/2+ 2 ) and third (5/2+ 1 ) excited states.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' As in experimental data, the theory predicts a staggering between the two fomer and two latter states but the relative spacing between the two pairs of levels, as well as the spacing between the levels within a pair, are too large.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' The 5/2+ 2 and 7/2+ 1 states also appear in our calculations but at too high excitation energy.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' The low-lying spectrum of positive parity states of 197Au has been interpreted with De-Shalit’s core-excitation model of odd-mass nuclei [47], within which an odd- even nucleus is treated as a single nucleon coupled to an even-even core.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Whenever the excitation of the core is energetically favored compared to the promotion of the single nucleon to a higher orbital, in this model the lowest lying excited states of the odd-even nucleus can be interpreted as the single-particle configuration of the 5 ground state coupled in different ways to the lowest excitation of the even-even core.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' When applied to 197Au [6,48–51], the ground state of the nucleus is constructed as a proton 2d3/2 particle (hole) coupled to a 196Pt (198Hg) core with Jπ = 0+.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='3 Then, the weak coupling of the same 2d3/2 particle, or hole, to the Jπ = 2+ excited state of the (appropriate) core generates a quartet of state with Jπ = 1/2+, 3/2+, 5/2+, 7/2+ whose energy centroid Ec = {� J(2J + 1)E(Jπ)} / {� J(2J + 1)} is equal to the energy E(2+) of the excited core [52].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Using the experimental excitation energies, we obtain Ec = 364.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='2 keV that is close to the values of E(2+) = 355.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='7 keV and for 411.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='8 keV for 196Pt and 198Hg, respectively.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Computing the energy centroid within our approach, we obtain the value Ec = 630.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='7 keV that is obviously too large compared to the experimental one but should be compared the theoretical values of E(2+) for the neighboring even-even nuclei calculated within the same theoretical framework, which is technically possible but falls outside the scope of the present article.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' The MR-EDF theory also correctly predicts the 11/2− 1 state to be lowest state of negative parity but with an excitation energy of 792 keV, about 400 keV too high compared to the experimental value of 409 keV.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' This is especially surprising given that the energy difference between the AMPNR minima for Jπ = 3/2+ and 11/2− has the correct order of magnitude as can be seen Figs.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' As a matter of fact, the minimum for Jπ = 11/2− has roughly the same energy as the one for Jπ = 1/2+.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' What happens is that during the configuration mixing, the 11/2− 1 state does not gain nearly as much correla- tion energy as the positive parity states and, therefore, ends up at a too high excitation energy.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' It is not en- tirely clear why the mixing is less important in this case.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' It might be due to the deficiency of the effective interaction but we can not exclude the possibility that other factors may play a role.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' For example, we had to use more restrictive values for the cutoffs before and after K-mixing to remove states not well represented on our Cartesian mesh.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Therefore, it is possible that some important components or non-diagonal matrix elements suffer from numerical inaccuracy.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Another possibility is that our selection strategy for the one-quasi-particle to self-consistent block at the mean-field level misses some configurations with negative parity relevant in the subsequent shape mixing.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' In general, the theoretical spectrum is too spread in energy, which is an often-encountered deficiency of MR- EDF calculations based on reference states generated by 3We mention in passing that some authors argue that using a 198Hg core provides a better global description of experimental data [6].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Quantity Experiment Theory E(3/2+ 1 ) 1559.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='384 1556.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='044 rrms(3/2+ 1 ) 5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='4371(38) 5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='389 µ(1/2+ 1 ) +0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='416(3) +0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='01 µ(3/2+ 1 ) +0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1452(2) 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='38 µ(5/2+ 1 ) +0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='74(6) +0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='15 µ(5/2+ 2 ) +3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='0(5) +0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='14 µ(7/2+ 1 ) +0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='84(7) +0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='51 µ(9/2+ 1 ) +1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='5(5) +0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='81 µ(11/2− 1 ) (+)5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='96(9) +6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='87 Qs(3/2+ 1 ) +0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='547(16) +0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='65 Qs(11/2− 1 ) +1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='68(5) +2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='05 Table 1: Spectroscopic quantities for the low-lying states of 197Au: total energy E (MeV), root-mean-square (rms) charge radius rrms (fm), magnetic dipole moments µ (µN), and spectroscopic quadrupole moments Qs (eb).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Experimental data are taken from [11,12,55–57].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' The experimental error on the binding energy is much smaller than the rounded value given here a variation of the total energy without consideration for the angular momentum of the trial states.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Indeed, such a variation tend to energetically favor the ground state.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' This deficiency can be in principle corrected by adding a constraint on the average angular momentum of the trial states during the minimization and using the value of the constraint as an additional generator coordinate.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Unfortunately, such calculations are computationally expensive and very few practical applications exist [53, 54].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' In Table 1, we report spectroscopic quantities for some of the low-lying states.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' First, we see that the calcu- lations reproduce fairly well the binding energy and root-mean-square charge radius of the ground state, with a relative accuracy below 1%.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' The spectroscopic quadrupole moments for the 3/2+ 1 and 11/2− 1 states are also reasonably well described in spite of being slightly too large.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' While we indicate in Table 1 the value for spectroscopic quadrupole moment of the ground state, Qs(3/2+ 1 ) = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='547(16) eb, currently taken as the accepted value in the compilation of Ref.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' [58], and which was determined using muonic hyperfine measur- ments [51], we remark that other values appear in the literature that are slightly larger, i.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='60 eb and 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='64 eb in Ref.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' [59] and 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='59 eb in Ref.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' [60], and in better agreement with the value of 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='65 eb obtained in our calculations.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Concerning the magnetic moments, they are, overall, poorly described.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' The values of most of them are sig- nificantly underestimated in our calculations and the 6 Transition Type Experiment Theory 1/2+ 1 → 3/2+ 1 E2 35(3) 45 M1 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='004 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='019 3/2+ 2 → 1/2+ 1 E2 18(3) 6 M1 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='089(9) 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='048 3/2+ 3 → 1/2+ 1 E2 9 M1 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='34 3/2+ 2 → 3/2+ 1 E2 18.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='5(19) 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='4 M1 < 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='001 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='002 3/2+ 3 → 3/2+ 1 E2 4 M1 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='02 5/2+ 1 → 1/2+ 1 E2 14.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='4(17) 12 5/2+ 1 → 3/2+ 1 E2 26(6) 30 M1 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='034(4) 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='065 5/2+ 2 → 1/2+ 1 E2 7.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='6(23) 8 5/2+ 2 → 3/2+ 1 E2 7(6) 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='4 M1 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='083(10) < 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='001 7/2+ 1 → 5/2+ 1 E2 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='18(7) 1 M1 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='012(1) 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='106 7/2+ 1 → 3/2+ 1 E2 33(3) 38 7/2+ 1 → 3/2+ 2 E2 6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='8(20) 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='3 7/2+ 1 → 3/2+ 3 E2 3 7/2+ 2 → 3/2+ 2 E2 6(4) 22 7/2+ 2 → 3/2+ 3 E2 2 7/2+ 2 → 5/2+ 1 E2 21(6) 13 M1 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='175(23) 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='010 9/2+ 1 → 7/2+ 1 E2 10(7) 10 M1 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='028(10) 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='047 9/2+ 1 → 5/2+ 1 E2 41(5) 43 Table 2: Reduced transition probabilities among the low-lying state of 197Au given in Weisskopf units.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Ex- perimental data are taken from [46], which are based on the evaluation [3] moment of the ground state has even the wrong sign.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Surprisingly, the best (relative) agreement with exper- imental data is obtained for the magnetic moment of the 11/2− 1 state.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' A similar mediocre description of the magnetic moments was already observed in our study of the 128,129,130Xe nuclei and we refer to this article [34] for a discussion of the large spectrum of possible reasons for this problem that is faced by the vast majority of EDF calculations of magnetic properties.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' In Table 2, we compare the theoretical values for the reduced transition probabilities B(E2) and B(M1) to available experimental data.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Concerning the E2 transi- tions, the theory gives reasonable estimates for most of the decays.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' In particular, all of the strong transitions, i.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 1/2+ 1 → 3/2+ 1 , 5/2+ 1 → 3/2+ 1 , 7/2+ 1 → 3/2+ 1 and 9/2+ 1 → 5/2+ 1 , are well described.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' More generally, the hierarchy between the transitions seems to be respected, i.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' strong (weak) experimental transitions tend to be strong (weak) in our calculations.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' One notable excep- tion are the transitions towards/from the 3/2+ 2 state that are largely underestimated in our calculations.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' A possible interpretation is that the 3/2+ 2 and 3/2+ 3 states are inverted in our calculation compared to the experi- mental spectrum.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Indeed, in Table 2 we also report the calculated transitions towards/from the 3/2+ 3 state that are in better agreement with the experimental data for the transitions towards/from 3/2+ 2 state.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' In the limit case of the core-excitation model discussed above, the reduced transition probabilities from the states of quar- tet 1/2+ 1 , 3/2+ 2 , 5/2+ 1 , 7/2+ 1 to the 3/2+ 1 ground state are supposed to be equal among each other and with the B(E2 : 2+ 1 → 0+ 1 ) of the even-even core.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Obviously, these equalities are not verified exactly for experimen- tal data but the values remain somewhat close.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='4 In particular, within the same model, the electromagnetic transition probabilities are very sensitive to the mixing of the Jπ = 3/2+ intrinsic states [48], a problem that might also be present in our approach.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Concerning the M1 transitions, the model performs poorly and most of the probabilities are either widely underestimated or widely overestimated.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' These lacking results are consistent with the observation made above on the magnetic moments.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Again, this characteristic is a deficiency found in many nuclear EDF calculations.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' While the projection techniques used here are crucial for the reliable and unambiguous comparison of calculated and experimental data for magnetic properties, they do by themselves not lead to a satisfying description of data.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' We refer again to [34] for further discussion of this issue.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='3 Collective wave functions We now turn our attention towards the analysis of the collective wave functions gJπ σ (β, γ) of the correlated states as defined in Ref.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' [34].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' We recall here that the squared collective wave functions (scwf) is a quantity that can be used to gauge the importance of a given deformation in the correlated wave function obtained in the final step of the MR-EDF calculations, with the caveat that, strictly speaking, it cannot be interpreted as a probability distribution due to the non-orthogonality of the reference states in the set.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' In Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 4, we display the scwf for several low-lying states of 197Au.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Interestingly, in all cases, the distribution of the scwf squared is dominated by triaxial shapes, 4We mention that the B(E2 : 2+ 1 → 0+ 1 ) values are 40.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='6(20) and 28.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='8(4) W.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='u.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' for 196Pt and 198Hg, respectively [46,61,62].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 7 Jπσ = 1/2+1 Jπσ = 3/2+1 Jπσ = 3/2+2 Jπσ = 3/2+3 Jπσ = 5/2+1 Jπσ = 5/2+2 Jπσ = 7/2+1 Jπσ = 7/2+2 Jπσ = 9/2+1 Jπσ = 11/2− 1 Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 4: Collective wave function squared for several low-lying states of 197Au with different values of Jπ σ .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Black lines are separated by 10% of the (respective) maximum value indicated by a silver star with a sharply peaked maximum that has a quadrupole deformation of β ≃ 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='14.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' But depending on the value of Jπ σ , the maximum is either located at angle γ ≈ 40◦ or γ ≈ 20◦.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' In particular, we remark that the scwf of the 3/2+ 1 and 3/2+ 2 states exhibit different behaviour with the former being located closer to the oblate axis whereas the latter favours the prolate side of the sextant.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Also, the scwf of the 3/2+ 3 state is very similar to the one of the 3/2+ 1 state.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' This is interesting for two reasons.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' First, it is contrary to what could have been expected looking at the AMPNR energy surface for Jπ = 3/2+ in Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Second, this is consistent with the oblate-like behavior expected in an independent-particle model for a nucleus close to the Z = 82 and N = 126 shell closures.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Still, it is important to stress that non-axial deformations carry a substantial percentage of the scwf.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Looking more closely at the scwfs of the positive parity states, we can arrange them into three groups of similar appearance: a) the states 1/2+ 1 , 3/2+ 1 , 3/2+ 3 and 7/2+ 1 that have a scwf mostly located in the range 30◦ ≤ γ ≤ 60◦ b) the states 3/2+ 2 , 5/2+ 2 and 7/2+ 2 that have a scwf mostly located in the range 0◦ ≤ γ ≤ 30◦ and c) the states 5/2+ 1 and 9/2+ 1 whose scwf are more evenly distributed as a function of γ and seem a combination of the cases a) and b).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' This is in good agreement with the data for the reduced transition probabilities given in Table 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Indeed, the transitions between the states of a given group have very large B(E2) values whereas the transitions between the states belonging to a different group are less likely.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' This is not a perfect rule, however, because the 5/2+ 1 state has also an strong transition towards the 3/2+ 1 ground state but not towards the 1/2+ 1 excited state even if the scwfs of the two latter states have similarities.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' To come back to the core-excitation model analysis, the fact that the scwf of the 1/2+ 1 , 3/2+ 3 ,5 5/2+ 1 and 7/2+ 1 excited states have a large overlap with 5Provided that we interpret the 3/2+ 2 and 3/2+ 3 states as being inverted in our calculations compared to experimental data.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 8 the scwf of the 3/2+ 1 ground state is consistent with the interpretation of the quartet of positive parity state as being weak coupling of the same single-particle state to a collective even-even core with an angular momentum of either Jπ = 0+ or 2+.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' As a last comment, we remark that the scwf of the 11/2− 1 state has a narrower distribution than the other ones displayed, which is consistent with the fact that this state does not mix as much when diagonalizing the Hamiltonian within the space spanned by the symmetry- projected reference states.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='4 Average deformation Finally, following the strategy presented in our previous article on xenon isotopes [34], we use the scwf to compute deformation parameters for the 3/2+ 1 ground state of 197Au and obtain: an average elongation of ¯β(3/2+ 1 ) = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='13, with a standard deviation of ∆β(3/2+ 1 ) = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='03, and an average angle of ¯γ(3/2+ 1 ) = 40◦, with a standard deviation of ∆γ(3/2+ 1 ) = 15◦.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' This average deformation is consistent with the distribution displayed in Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 4 as the maximum is located at a deformation of β = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='14 and γ = 41◦ but the distribution extends towards smaller values of β and is more or less equally distributed with respect to the γ = 40◦ axis.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Within the rigid rotor model, it is also possible to com- pute a deformation βr for the 0+ 1 ground state of an even-even nucleus using the experimental B(E2) values, for more details see for example Refs.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' [34,63].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Comput- ing βr for the even-even nuclei adjacent to 197Au one obtains the value 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='13 for 196Pt and 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='11 198Hg.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Our average deformation ¯β(3/2+ 1 ) = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='12 fits nicely between these two values, although we have to mention that the definitions of the two elongations are model depen- dent such that this excellent agreement may be partly accidental.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' The results of axially-symmetric EDF calculations based on the Gogny D1S parametrization [15,16] reported in the AMEDEE database [17] indicate a sharp minimum at a deformation of about β ≈ 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='12 for 197Au.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' This is perfectly consistent with our estimate.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' The AMEDEE database also reports average deformations obtained from large-scale five-dimensional collective Hamiltonian (5DCH) calculations of even-even nuclei throughout the nuclear chart [64].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' We recall here that the 5DCH can be derived as an approximation to the full GCM performed here [63].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' While their definition for the average deforma- tion differs from ours, we mention that for 196Pt (198Hg), they obtain an average elongation of 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='135 (0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='110), with a standard deviation of 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='032 (0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='030), and average angle of 32◦ (31◦), with a standard deviation of 12◦ (12◦).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' If the values for the elongation are consistent with our result, the average angles differ slightly with the 5DCH result indicating a deformation right at the center of the triaxial plane, although the fluctuations are large enough such that the results are compatible.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 3 Heavy-ion collisions As previously mentioned, knowing the structure of 197Au is of particular relevance in the context of high-energy nuclear experiments, as gold is the primary species col- lided at the BNL RHIC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' This section analyzes the con- sequences of our results for model simulations of ultra- relativistic 197Au+197Au collisions.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1 Woods-Saxon parameterization of the ground state Traditionally, simulations of high-energy nuclear col- lisions take as input from nuclear structure a point- nucleon density which is used to sample nucleon coordi- nates and define an interaction region between two ions on a collision-by-collision basis.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='6 The standard choice for the nucleon density is that of a deformed Woods-Saxon (WS) profile: ρ(r, θ, φ) = ρ0 1 + e[r−R(θ,φ)]/a , (1) where r, θ, φ are the usual spherical coordinates, ρ0 is the saturation density, a is the surface diffuseness and R(θ, φ) is the nuclear radius parameterized as R(θ, φ) = R0 � 1 + βWS 2 � cos(γWS)Y20(θ, φ) (2) + √ 2 sin(γWS)Re � Y22(θ, φ) �� + βWS 4 Y40(θ, φ) � , where the spherical harmonics Ylm(θ, φ) are in complex form.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Note that the shape parameters βWS 2 , γWS and βWS 4 represent surface deformations that differ from the volume deformation reported in the analysis of the previous sections [69].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' We consider now the intrinsic shape of 197Au computed from a single Hartree-Fock-Bogoliubov (HFB) calcula- tion with the SLyMR1 interaction in which the expecta- tion value of the quadrupole operators are constrained 6More sophisticated calculations based on nuclear configura- tions obtained from ab initio nuclear theory have also been recently performed [65–68].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' For the moment, they are limited to the description of collisions of 16O ions.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 9 Parameter Proton Neutron Nucleon ρ0 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='067 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='090 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='157 R0 6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='44 6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='65 6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='56 a 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='46 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='49 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='48 βWS 2 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='134 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='137 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='135 γWS 43◦ 43◦ 43◦ βWS 4 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='024 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='023 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='023 Table 3: Parameters for the point-proton, point-neutron and point-nucleon densities defined as in Eq.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' (1) and fitted to reproduce the one-body densities of a quasi- particle state constrained to have, on average, β = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='13 and γ = 40◦;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' see the body of the text for more details.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' The parameters R0 and a are given in units of fm, whereas ρ0 is given in units of fm−3 Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 5: Schematic illustration of the shape of 197Au based on the surface parametrization of the matter density of Eq.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' (2), and using the parameters reported in Tab.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 3 such that the one-body density of the trial one-quasi- particle state7 verifies, on average, β = ¯β(3/2+ 1 ) = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='13 and γ = ¯γ(3/2+ 1 ) = 40◦.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='8 We fit the resulting one- body nucleon density with the Woods-Saxon profile given in Eq.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' (1).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' The fit parameters are reported in Tab.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' We obtain, thus, a new microscopically mo- tivated parametrization for the Woods-Saxon profile representing the nucleon density of the ground state of 197Au which can be employed in simulations of high- energy collisions.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' This profile corresponds to a triaxial ellipsoid with radii 6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='02 fm, 6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='68 fm, and 6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='97 fm, as illustrated in Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 7The trial one-quasi-particle state is built by blocking a single- particle state originating from the spherical 2d3/2 shell.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 8All other non-vanishing multipole moments authorized by the symmetries of our calculations are let free to adopt a value that minimizes the total energy of the trial quasi-particle state.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' For completeness, we evaluate as well the neutron skin of the intrinsic shape, as defined by the difference of rms radii, ∆rnp = ⟨r2⟩1/2 n −⟨r2⟩1/2 p .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' For the density returned by the constrained HFB calculation, we find ∆rnp[HFB(¯β, ¯γ)] = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='17 fm, (3) which is in perfect agreement with the result obtained from the full MREDF calculation ∆rnp[MREDF] = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='17 fm.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' (4) On the other hand, the fitted Woods-Saxon profile gives a neutron skin ∆rnp[WS fit] = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='19 fm, (5) meaning that, even for a large nucleus such as 197Au, the Woods-Saxon parametrization does not fully capture skin differences of order 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1 fm between neutrons and protons.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' We note that both the above estimates agree with a recent measurement of the STAR collaboration obtained via diffractive photo-production of ρ0 mesons in ultra-peripheral 197Au+197Au collisions [70], ∆rnp[STAR] = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='17 ± 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='03 (stat.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=') ± 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='08 (syst.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=') fm.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' (6) We note, in addition, that the half-width radius obtained for 197Au by the STAR collaboration, R0[STAR] = 6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='53 ± 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='06 fm, is fully consistent with that exhibited by our nucleon density, R0[WS fit] = 6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='56 fm.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' This suggests that the density of gluons relevant for scattering at these beam energies is in fact very close to the rest- frame point-nucleon density.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' This potentially adds to the circumstantial evidence of a small nucleon width in high-energy collisions mediated by gluons [71–75].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' We discuss now the observational consequences of our newly-derived nucleon density for relativistic 197Au+197Au collisions.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Model calculations of such processes (see e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='g.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Ref.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' [76] for a state-of-the-art Bayesian analysis) have so far employed the charge density of the nucleus, as inferred from low-energy electron-nucleus scattering ex- periments [77], as a proxy for the nucleon density.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' The corresponding radial profiles are R0 = 6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='38 fm, and a = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='53 fm.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Nuclear quadrupole deformation has been instead included by simply implementing βWS 2 = −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='13, as reported by finite-range liquid drop model evalua- tions [78].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' In terms of radial profiles, there are, thus, minor differences between the WS parametrization that we show in Tab.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 3 and that implemented in the lit- erature.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' We only note a reduction by 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='05 fm in the diffuseness parameter, a, which is due to the inclusion of the neutron density.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' This will have a mild, though visible impact on the initial eccentricities, εn, of the sys- tem [79–81].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' A new feature of our calculation is instead the fact that 197Au is not fully oblate, but presents γWS = 43◦.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' We investigate now the impact of such a feature on high-energy collisions.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 10 cm 100% x1013 6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='02 fm 6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='68 fm 6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='97 fm10 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='2 Impact of the triaxiality In the context of multi-particle correlation measure- ments in the soft sector of high-energy nuclear colli- sions, the strongest sensitivity to the triaxial structure of the colliding nuclei is carried by the mean momentum- elliptic flow correlation [82–84], ρ2 ≡ ρ(⟨pt⟩, v2 2) = ⟨⟨pt⟩v2 2⟩ − ⟨⟨pt⟩⟩⟨v2 2⟩ σ(⟨pt⟩)σ(⟨v2 2⟩) , (7) where outer brackets denote a statistical average over events, and σ(o) is the standard deviation of observable o.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' This quantity can be evaluated in the final states as a three-particle correlation [85], and it measures the strength of the statistical correlation between the charged-particle average transverse momentum, ⟨pt⟩, and the charged-particle elliptic flow, v2, at a given collision multiplicity.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' To assess the impact of γWS = 43◦ on the ρ2 correlator of 197Au+197Au collisions, we follow Ref.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' [30] and provide an estimate of the measured ρ2 from high-statistics simu- lations of the initial condition of these processes.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' For the details of such simulations, we refer to the exhaustive de- scriptions given in Ref.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' [30].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Briefly, we assume that the distribution of final-state multiplicities is proportional to the distribution of initial-state entropy, S, which we calculate event-to-event following the original TRENTo parametrization [86] (s(x, τ0) ∝ √TATB, S = � d2x s) with a nucleon size w = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='5 fm, and a fluctuation pa- rameter, k, tuned to reproduce measured multiplicity histograms in 208Pb+208Pb collisions at CERN LHC energy.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' We consider that i) the mean transverse momen- tum is, at a given entropy, proportional to the initial E/S, where E is the total energy of the system [87,88], obtained upon application of the equation of state of high-temperature QCD (e(x) ∝ s(x)4/3, E = � d2x e), and ii) that the elliptic flow is proportional to the initial eccentricity of the system, ε2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' The Pearson correlation coefficient of Eq.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' (7) can then be estimated by replac- ing v2 2 and ⟨pt⟩ with, respectively, ε2 2 and E/S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Note that the resulting estimator should not be compared directly to the experimental measurements, as it misses effects related to the cuts in transverse momentum, pt, implemented in the experimental analysis, which have been shown to be sizable for the magnitude of this observable [31,89,90].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' That said, it is the initial-state estimator that carries the dependence on the deforma- tion parameters, such that the relative impact of the value of γWS on the final-state result can be assessed from it [30,91].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' We perform 20 × 106 minimum bias simulations of 197Au+197Au collisions for three structure scenarios, 300 350 400 450 500 550 600 Nrec ch (|η| < 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='5) 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='00 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='05 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='10 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='15 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='20 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='25 ρ � ⟨pt⟩, v2 2 � ← uncertainty on STAR data at Nrec ch ≈ 550 TRENTo, 200 GeV Au+Au oblate gold (βWS 2 = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='135, γWS = 60◦) triaxial gold (βWS 2 = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='135, γWS = 43◦) prolate gold (βWS 2 = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='135, γWS = 0) 16 9 3 1 centrality (%) Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 6: Initial-state estimates of ρ(⟨pt⟩, v2 2) in 200 GeV 197Au+197Au collisions for prolate ions (dot-dashed line), oblate ions (dotted line) and triaxial ions (dashed line) presenting γWS = 43◦, as a function of the number of reconstructed charged tracks in the STAR detector.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Shaded bands (of the same width as the lines) are statis- tical uncertainties.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' The figure reports as well the total uncertainty on preliminary STAR measurements for this observable at high multiplicities.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' namely, we set βWS 2 = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='135, and consider γWS = 0◦, 43◦, and 60◦.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='9 Rescaling the TRENTo entropy to match the observed mutliplicity of reconstructed charged tracks in the STAR detector, N rec ch , at midrapidity (|η| < 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='5), our results for ρ2 are reported in Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Qualitatively, the impact of γWS follows the generic parametric expec- tation ρ2 ∝ c0 − c1(βWS 2 )3 cos(3γWS), where c0 and c1 are positive coefficients [30,91].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' We conclude that a 17◦ deviation from oblateness in 197Au leads to a correction of order 10-15% to ρ2 for collisions in the 0-2% centrality range.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' We reiterate that, while our results for the magni- tude of the Pearson coefficient should not be compared directly to data, we expect the correction induced by the triaxiality, relative to the oblate scenario, to be ro- bustly captured by our initial-state evaluation.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' In Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 6 we report as well the size of the experimental error on preliminary ρ2 data at high multiplicity from the STAR collaboration [92].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' The error bar turns out to be signifi- cantly smaller than the splitting that we find between the triaxial scenario (red dashed line) and the oblate scenario (dotted blue line).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Therefore, according to our results the impact of the triaxiality has been already iso- lated in the preliminary data, and it will be possible to 9We safely neglect the effect of the very small hexadecapolarity of the nucleus, βWS 4 = −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='023, in these simulations.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 11 quantify it in the future via high-precision hydrodynamic simulations.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' We stress, though, that the most effective way to access the value of γWS is by studying the ρ2 correlator of 197Au+197Au collisions normalized with that of 238U+238U collisions, as done in Refs.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' [30, 31] to extract such an information in the comparisons of 129Xe+129Xe and 208Pb+208Pb collisions, which allows one to fully cancel theoretical and experimental system- atical uncertainties and isolate transparent information about the nuclear structure.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' The current mismatch be- tween hydrodynamic results and experimental data for 238U+238U collisions [93] prevents us, for the moment, from performing such an analysis, which will be thus reported in future work.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 4 Conclusions In the present article, we first reported on new re- sults on the low-energy structure of the heavy odd- mass nucleus 197Au obtained by performing state-of- the-art MR-EDF calculations that include the mixing of angular-momentum and particle-number projected Bogoliubov quasi-particle states with different average triaxial shapes.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' All the calculations were realized using the parametrization SLyMR1 of a Skyrme-type pseudo- potential [44,94].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Although odd-mass nuclei represent half of the existing nuclei in the nuclear chart, their calculations within the full-fledged MR-EDF framework are still scarce, ex- ceptions being [34,40,41,95].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' In this work, to generate reference states adapted to the modeling of odd-mass nuclei, we performed self-consistent blocking of Bogoli- ubov one-quasi-particle states and considered exactly all the time-odd terms of the functional.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' The results obtained on the low-energy spectroscopy of 197Au are reasonable.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' The spin-parity assignments for the 3/2+ 1 ground state and for the first few excited states are correct even if the levels are too spread out, a well-known deficiency of usual MR-EDF calculations that can be corrected by adding a supplemental con- straint on the average angular momentum of the trial wave functions when generating the set of reference states to be projected and mixed [53,54].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' The binding energy, root-mean-square charge radius and spectro- scopic quadrupole moment of the of the ground state are also well reproduced.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' By contrast, the calculations fail to reproduce the known magnetic moments for the ground and excited states.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Concerning the electromag- netic transitions, the values for the reduced transition probabilities B(E2) are, overall, well described whereas the values for the B(M1) are off, sometimes by more than one order of magnitude.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Starting from the collective wave function of the ground state, we computed average triaxial deformation param- eters ¯β(3/2+ 1 ) = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='13 and ¯γ(3/2+ 1 ) = 40◦.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Following the the strategy of Ref.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' [30], we then fitted the parameters of a deformed Woods-Saxon density profile, to obtain a new state-of-the-art microscopically-motivated input for the simulation of high-energy 197Au+197Au colli- sions.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' In terms of radial profile parameters, our result corrects to some extent the widely- and incorrectly- employed charge-density parametrization, which has in particular a too large skin thickness.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' For future precision phenomenological studies of 197Au+197Au collisions, es- pecially in view of the upcoming sPHENIX program at the BNL RHIC, it will be crucial to implement real- istic properties of the point-nucleon density in Monte Carlo simulations.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' This includes as well implementing an appropriate triaxiality, of order 45◦, for gold ions.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Our estimates indicate that this magnitude of the tri- axiality does impact the final state in a significant way, and we expect future theoretical work to be able to cleanly isolate such a contribution from the data.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' As an outlook, we emphasize that measurements of the third centered moment (skewness) of the distribution of ⟨pt⟩ [96] provide additional and independent information about γWS [91], and can be used in conjunction with hydrodynamic simulations to further test our prediction for this parameter.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Acknowledgements We thank Chunjian Zhang for help with the entropy-to-multiplicity conversion used in Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 6, and Wouter Ryssens for useful discussions.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' This project has re- ceived funding from the European Union’s Horizon 2020 re- search and innovation programme under the Marie Sk�lodowska- Curie grant agreement No.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 839847.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' acknowledges sup- port by the Agence Nationale de la Recherche, France, un- der grant No.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 19-CE31-0015-01 (NEWFUN).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' is funded by the Deutsche Forschungsgemeinschaft (DFG, German Re- search Foundation) under Germany’s Excellence Strategy EXC2181/1-390900948 (the Heidelberg STRUCTURES Ex- cellence Cluster), within the Collaborative Research Center SFB1225 (ISOQUANT, Project-ID 273811115).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' The calcula- tions were performed by using HPC resources from CIEMAT (Turgalium), Spain (FI-2021-3-0004, FI-2022-1-0004).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' References 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Geiger, E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Marsden, E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rutherford, On a diffuse reflection of the α-particles, Proceedings of the Royal Society of London.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Series A, Containing Papers of a Math- ematical and Physical Character 82 (557) (1909) 495–500.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' arXiv:https://royalsocietypublishing.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/pdf/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 1098/rspa.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1909.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='0054, doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1098/rspa.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1909.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='0054.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://royalsocietypublishing.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/abs/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 1098/rspa.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1909.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='0054 12 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rutherford, Lxxix.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' the scattering of α and β par- ticles by matter and the structure of the atom, The London, Edinburgh, and Dublin Philosophical Maga- zine and Journal of Science 21 (125) (1911) 669–688.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' arXiv:https://doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1080/14786440508637080, doi: 10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1080/14786440508637080.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1080/14786440508637080 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' X.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Huang, C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Zhou, Nuclear data sheets for A=197, Nu- clear Data Sheets 104 (2) (2005) 283–426.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:https: //doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1016/j.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='nds.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='2005.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='01.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='001.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://www.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='sciencedirect.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='com/science/article/ pii/S0090375205000025 4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Elliott, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Wulff, Hyperfine structure of gold, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 55 (1939) 170–175.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='55.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='170.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='55.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='170 5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' F.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Cook, C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Class, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' T.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Eisinger, Electric excitation of 197Au, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 96 (1954) 658–663.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/ PhysRev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='96.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='658.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='96.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='658 6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Bolotin, D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Kennedy, B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Linard, A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Stuchbery, S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Sie, I.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Katayama, H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Sakai, Measured lifetimes of states in 197Au and a critical comparison with the weak-coupling core-excitation model, Nuclear Physics A 321 (1) (1979) 231–249.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:https://doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1016/0375-9474(79) 90696-1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://www.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='sciencedirect.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='com/science/article/ pii/0375947479906961 7.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Stuchbery, L.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Wood, H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Bolotin, C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Doran, I.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Mor- rison, A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Byrne, G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Lampard, Measured gyromagnetic ratios and the low-excitation spectroscopy of 197Au, Nu- clear Physics A 486 (2) (1988) 374–396.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:https: //doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1016/0375-9474(88)90242-4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://www.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='sciencedirect.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='com/science/article/ pii/0375947488902424 8.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' N.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Fotiades, R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' O.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Nelson, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Devlin, K.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Starosta, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Becker, L.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Bernstein, P.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Garrett, W.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Younes, States in 197Au from the (n, n ′γ) reaction, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' C 71 (2005) 064314.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='71.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='064314.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='71.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 064314 9.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Wheldon, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Valiente-Dob´on, P.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Regan, C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Pearson, C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Y.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Wu, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' F.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Smith, A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' O.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Macchiavelli, D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Cline, R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Chakrawarthy, R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Chapman, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Cromaz, P.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Fallon, S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Freeman, W.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Gelletly, A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' G¨orgen, A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Hayes, H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Hua, S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Langdown, I.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Y.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Lee, X.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Liang, Z.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Podoly´ak, G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Sletten, R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Teng, D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Ward, D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Warner, A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Yamamoto, Observation of an isomeric state in 197Au, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' C 74 (2006) 027303.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='74.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='027303.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='74.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 027303 10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' N.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Fotiades, R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' O.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Nelson, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Devlin, S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Holloway, T.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Kawano, P.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Talou, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Chadwick, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Becker, P.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Garrett, Feeding of the 11/2− isomers in stable Ir and Au isotopes, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' C 80 (2009) 044612.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='80.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='044612.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='80.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 044612 11.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' N.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Stone, Table of recommended magnetic dipole moments: Part I, Long-lived states, INDC(NDS)-0794 (2019).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://www-nds.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='iaea.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/publications/indc/ indc-nds-0794.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='pdf 12.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' N.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Stone, Table of recommended magnetic dipole moments: Part II, Short-lived states, INDC(NDS)-0816 (2020).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://www-nds.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='iaea.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/publications/indc/ indc-nds-0816.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='pdf 13.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' ˚A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Bohr, B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Mottelson, Nuclear structure, volume I and II, World Scientific Publishing, Singapore, 1998.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 14.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' I.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Hamamoto, B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Mottelson, Further exami- nation of prolate-shape dominance in nuclear deformation, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' C 79 (2009) 034317.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='79.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='034317.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='79.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 034317 15.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Decharg´e, D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Gogny, Hartree-Fock-Bogolyubov calculations with the D1 effective interaction on spherical nuclei, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' C 21 (1980) 1568–1593.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='21.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1568.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='21.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 1568 16.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Berger, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Girod, D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Gogny, Time-dependent quan- tum collective dynamics applied to nuclear fission, Com- puter Physics Communications 63 (1) (1991) 365–374.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:https://doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1016/0010-4655(91)90263-K.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://www.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='sciencedirect.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='com/science/article/ pii/001046559190263K 17.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Hilaire, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Girod, Large-scale mean-field calculations from proton to neutron drip lines using the D1S Gogny force, The European Physical Journal A 33 (2) (2007) 237–241.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1140/epja/i2007-10450-2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1140/epja/i2007-10450-2 18.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Adams, et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=', Experimental and theoretical challenges in the search for the quark–gluon plasma: The star col- laboration’s critical assessment of the evidence from rhic collisions, Nuclear Physics A 757 (1) (2005) 102–183, first Three Years of Operation of RHIC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:https: //doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1016/j.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='nuclphysa.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='2005.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='03.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='085.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://www.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='sciencedirect.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='com/science/article/ pii/S0375947405005294 19.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' K.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Adcox, et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=', Formation of dense partonic matter in rel- ativistic nucleus–nucleus collisions at rhic: Experimental evaluation by the phenix collaboration, Nuclear Physics A 757 (1) (2005) 184–283, first Three Years of Operation of RHIC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:https://doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1016/j.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='nuclphysa.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='2005.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 03.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='086.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://www.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='sciencedirect.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='com/science/article/ pii/S0375947405005300 20.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Back, et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=', The phobos perspective on discover- ies at rhic, Nuclear Physics A 757 (1) (2005) 28–101, first Three Years of Operation of RHIC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:https: //doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1016/j.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='nuclphysa.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='2005.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='03.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='084.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://www.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='sciencedirect.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='com/science/article/ pii/S0375947405005282 21.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' I.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Arsene, et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=', Quark–gluon plasma and color glass condensate at RHIC?' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' the perspective from the brahms experiment, Nuclear Physics A 757 (1) (2005) 1–27, first Three Years of Operation of RHIC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:https: //doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1016/j.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='nuclphysa.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='2005.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='02.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='130.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://www.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='sciencedirect.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='com/science/article/ pii/S0375947405002770 22.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' L.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Miller, K.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Reygers, S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Sanders, P.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Steinberg, Glauber modeling in high-energy nuclear collisions, An- nual Review of Nuclear and Particle Science 57 (1) (2007) 205–243.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' arXiv:https://doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1146/annurev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='nucl.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 57.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='090506.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='123020, doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1146/annurev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='nucl.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='57.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='090506.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 123020.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1146/annurev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='nucl.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='57.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='090506.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 123020 13 23.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' W.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Busza, K.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rajagopal, W.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' van der Schee, Heavy ion collisions: The big picture and the big questions, Annual Review of Nuclear and Particle Science 68 (1) (2018) 339–376.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' arXiv: https://doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1146/annurev-nucl-101917-020852, doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1146/annurev-nucl-101917-020852.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1146/ annurev-nucl-101917-020852 24.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' L.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Adamczyk, et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=', Azimuthal anisotropy in U + U and Au + Au collisions at RHIC, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Lett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 115 (2015) 222301.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevLett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='115.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='222301.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevLett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 115.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='222301 25.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Acharya, et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=', Anisotropic flow in Xe-Xe collisions at √sNN = 5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='44 TeV, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Lett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' B 784 (2018) 82–95.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' arXiv:1805.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='01832, doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1016/j.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='physletb.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='2018.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='06.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='059.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 26.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Sirunyan, et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=', Charged-particle angular correla- tions in XeXe collisions at √sNN = 5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='44 TeV, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' C 100 (2019) 044902.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='100.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='044902.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='100.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 044902 27.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Aad, et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=', Measurement of the azimuthal anisotropy of charged-particle production in Xe + Xe collisions at √sNN = 5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='44 TeV with the ATLAS detector, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' C 101 (2020) 024906.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='101.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='024906.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='101.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 024906 28.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Abdallah, et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=', Search for the chiral magnetic effect with isobar collisions at √sNN = 200 GeV by the STAR collaboration at the BNL Relativistic Heavy Ion Collider, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' C 105 (2022) 014901.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='105.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='014901.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='105.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 014901 29.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Bally, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Brandenburg, G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Giacalone, U.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Heinz, S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Huang, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Jia, D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Lee, Y.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='-J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Lee, W.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Li, C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Loizides, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Luzum, G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Nijs, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Noronha-Hostler, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Ploskon, W.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' van der Schee, B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Schenke, C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Shen, V.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Som`a, A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Tim- mins, Z.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Xu, Y.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Zhou, Imaging the initial condition of heavy-ion collisions and nuclear structure across the nu- clide chart (2022).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='48550/ARXIV.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='2209.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='11042.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://arxiv.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/abs/2209.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='11042 30.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Bally, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Bender, G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Giacalone, V.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Som`a, Evi- dence of the triaxial structure of 129Xe at the large hadron collider, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Lett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 128 (2022) 082301.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevLett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='128.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='082301.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevLett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 128.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='082301 31.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' ATLAS, Correlations between flow and transverse mo- mentum in Xe+Xe and Pb+Pb collisions at the LHC with the ATLAS detector: a probe of the heavy-ion initial state and nuclear deformation (4 2022).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' arXiv:2205.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='00039.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 32.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' L.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Morrison, K.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Hady´nska-Kl¸ek, Z.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Podoly´ak, D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' T.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Doherty, L.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' P.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Gaffney, L.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Kaya, L.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Pr´ochniak, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Samorajczyk-Py´sk, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Srebrny, T.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Berry, A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Boukhari, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Brunet, R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Canavan, R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Catherall, S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Colosimo, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Cubiss, H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' De Witte, C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Fransen, E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Giannopoulos, H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Hess, T.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Kr¨oll, N.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Lalovi´c, B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Marsh, Y.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Palen- zuela, P.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Napiorkowski, G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' O’Neill, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Pakarinen, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' P.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Ramos, P.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Reiter, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rodriguez, D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rosiak, S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rothe, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rudigier, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Siciliano, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Sn¨all, P.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Spag- noletti, S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Thiel, N.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Warr, F.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Wenander, R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Zidarova, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Zieli´nska, Quadrupole deformation of 130Xe measured in a coulomb-excitation experiment, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' C 102 (2020) 054304.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='102.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='054304.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='102.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 054304 33.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Kisyov, C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Y.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Wu, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Henderson, A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Gade, K.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Kaneko, Y.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Sun, N.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Shimizu, T.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Mizusaki, D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rhodes, S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Biswas, A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Chester, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Devlin, P.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Farris, A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Hill, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Li, E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rubino, D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Weisshaar, Structure of 126,128Xe studied in coulomb excitation measurements, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' C 106 (2022) 034311.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='106.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='034311.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='106.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 034311 34.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Bally, G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Giacalone, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Bender, Structure of 128,129,130Xe through multi-reference energy density func- tional calculations, The European Physical Journal A 58 (9) (2022) 187.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1140/epja/s10050-022-00833-4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1140/epja/s10050-022-00833-4 35.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Bender, P.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='-H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Heenen, P.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='-G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Reinhard, Self-consistent mean-field models for nuclear structure, Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Mod.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 75 (2003) 121–180.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/RevModPhys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='75.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='121.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/RevModPhys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='75.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 121 36.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' N.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Schunck (Ed.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' ), Energy Density Functional Methods for Atomic Nuclei, 2053-2563, IOP Publishing, 2019.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi: 10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1088/2053-2563/aae0ed.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://dx.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1088/2053-2563/aae0ed 37.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Bender, P.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='-H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Heenen, Configuration mixing of angular-momentum and particle-number projected triaxial Hartree-Fock-Bogoliubov states using the Skyrme energy density functional, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' C 78 (2008) 024309.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='78.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='024309.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='78.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 024309 38.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' T.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rodr´ıguez, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' L.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Egido, Triaxial angular momentum projection and configuration mixing calculations with the Gogny force, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' C 81 (2010) 064323.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='81.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='064323.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='81.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 064323 39.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Yao, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Meng, P.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Ring, D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Vretenar, Configuration mixing of angular-momentum-projected triaxial relativis- tic mean-field wave functions, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' C 81 (2010) 044311.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='81.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='044311.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='81.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 044311 40.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Bally, B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Avez, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Bender, P.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='-H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Heenen, Beyond mean- field calculations for odd-mass nuclei, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Lett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 113 (2014) 162501.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevLett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='113.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='162501.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevLett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 113.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='162501 41.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Borrajo, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' L.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Egido, Ground-state properties of even and odd magnesium isotopes in a symmetry-conserving approach, Physics Letters B 764 (2017) 328–334.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi: https://doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1016/j.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='physletb.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='2016.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='11.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='037.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://www.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='sciencedirect.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='com/science/article/ pii/S0370269316307006 42.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Bally, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Bender, Projection on particle number and angular momentum: Example of triaxial bogoliubov quasiparticle states, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' C 103 (2021) 024315.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='103.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='024315.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='103.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 024315 43.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Sadoudi, T.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Duguet, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Meyer, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Bender, Skyrme functional from a three-body pseudopotential of second order in gradients: Formalism for central terms, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' C 88 (2013) 064326.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='88.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='064326.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='88.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 064326 44.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Jodon, Ph.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' thesis, Universit´e Claude Bernard - Lyon 1 (2014).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 14 45.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Baye, P.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='-H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Heenen, Generalised meshes for quantum mechanical problems, Journal of Physics A: Mathematical and General 19 (11) (1986) 2041–2059.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1088/ 0305-4470/19/11/013.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1088/0305-4470/19/11/013 46.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Data retrieved from the IAEA online nuclear data services.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://www-nds.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='iaea.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/ 47.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' de Shalit, Core excitations in nondeformed, odd-A, nuclei, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 122 (1961) 1530–1536.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='122.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1530.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='122.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 1530 48.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Braunstein, A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' De-Shalit, New evidence for core ex- citation in Au197, Physics Letters 1 (7) (1962) 264–266.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:https://doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1016/0031-9163(62)91375-6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://www.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='sciencedirect.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='com/science/article/ pii/0031916362913756 49.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' De-Shalit, Core excitation: Au197 revisited, Physics Letters 15 (2) (1965) 170–172.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:https://doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 1016/0031-9163(65)91327-2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://www.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='sciencedirect.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='com/science/article/ pii/0031916365913272 50.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' F.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' McGowan, W.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Milner, R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Robinson, P.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Stelson, Couloub excitation of 197Au and a core-excitation analy- sis, Annals of Physics 63 (2) (1971) 549–561.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:https: //doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1016/0003-4916(71)90028-5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://www.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='sciencedirect.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='com/science/article/ pii/0003491671900285 51.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Powers, P.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Martin, G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Miller, R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Welsh, D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Jenk- ins, Muonic 197Au: A test of the weak-coupling model, Nuclear Physics A 230 (3) (1974) 413–444.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:https: //doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1016/0375-9474(74)90147-X.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://www.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='sciencedirect.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='com/science/article/ pii/037594747490147X 52.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Lawson, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' L.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Uretsky, Center-of-gravity theorem in nuclear spectroscopy, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 108 (1957) 1300–1304.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='108.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1300.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='108.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 1300 53.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Borrajo, T.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rodr´ıguez, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' L.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Egido, Symme- try conserving configuration mixing method with cranked states, Physics Letters B 746 (2015) 341 – 346.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:https://doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1016/j.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='physletb.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='2015.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='05.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='030.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL http://www.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='sciencedirect.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='com/science/article/ pii/S0370269315003676 54.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' L.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Egido, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Borrajo, T.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rodr´ıguez, Collec- tive and single-particle motion in beyond mean field approaches, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Lett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 116 (2016) 052502.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevLett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='116.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='052502.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevLett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 116.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='052502 55.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' I.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Angeli, K.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Marinova, Table of experimental nuclear ground state charge radii: An update, Atomic Data and Nuclear Data Tables 99 (1) (2013) 69–95.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:https: //doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1016/j.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='adt.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='2011.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='12.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='006.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://www.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='sciencedirect.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='com/science/article/ pii/S0092640X12000265 56.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' W.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Huang, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Wang, F.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Kondev, G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Audi, S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Naimi, The AME 2020 atomic mass evaluation (I).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' evaluation of input data, and adjustment procedures, Chinese Physics C 45 (3) (2021) 030002.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1088/1674-1137/abddb0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1088/1674-1137/abddb0 57.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Wang, W.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Huang, F.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Kondev, G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Audi, S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Naimi, The AME 2020 atomic mass evaluation (II).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' tables, graphs and references, Chinese Physics C 45 (3) (2021) 030003.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1088/1674-1137/abddaf.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1088/1674-1137/abddaf 58.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' N.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Stone, Table of nuclear electric quadrupole moments, Atomic Data and Nuclear Data Tables 111-112 (2016) 1–28.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:https://doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1016/j.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='adt.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='2015.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='12.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='002.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://www.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='sciencedirect.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='com/science/article/ pii/S0092640X16000024 59.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' P.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Schwerdtfeger, R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Bast, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' L.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Gerry, C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Jacob, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Jansen, V.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Kell¨o, A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' V.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Mudring, A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Sadlej, T.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Saue, T.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' S¨ohnel, F.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Wagner, The quadrupole moment of the 3/2+ nuclear ground state of 197Au from electric field gradient relativistic coupled cluster and density-functional theory of small molecules and the solid state, The Journal of Chemical Physics 122 (12) (2005) 124317.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' arXiv:https: //doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1063/1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1869975, doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1063/1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1869975.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1063/1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1869975 60.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' W.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Itano, Quadrupole moments and hyperfine constants of metastable states of Ca+, Sr+, Ba+, Yb+, Hg+, and Au, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' A 73 (2006) 022510.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevA.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='73.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='022510.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevA.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='73.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 022510 61.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Xiaolong, Nuclear data sheets for A = 196, Nu- clear Data Sheets 108 (6) (2007) 1093–1286.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:https: //doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1016/j.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='nds.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='2007.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='05.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='001.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://www.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='sciencedirect.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='com/science/article/ pii/S0090375207000488 62.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' X.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Huang, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Kang, Nuclear data sheets for A = 198, Nuclear Data Sheets 133 (2016) 221–416.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:https: //doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1016/j.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='nds.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='2016.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='02.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='002.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://www.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='sciencedirect.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='com/science/article/ pii/S0090375216000156 63.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' P.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Ring, P.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Schuck, The Nuclear Many-Body Problem, Springer-Verlag, New York, 1980.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 64.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' P.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Delaroche, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Girod, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Libert, H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Goutte, S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Hilaire, S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' P´eru, N.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Pillet, G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' F.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Bertsch, Structure of even-even nuclei using a mapped collective hamiltonian and the D1S Gogny interaction, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' C 81 (2010) 014303.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='81.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='014303.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='81.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 014303 65.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Lim, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Carlson, C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Loizides, D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Lonardoni, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Lynn, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' L.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Nagle, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Orjuela Koop, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Ouel- lette, Exploring new small system geometries in heavy ion collisions, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' C 99 (2019) 044904.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='99.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='044904.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='99.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 044904 66.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rybczy´nski, W.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Broniowski, Glauber monte carlo pre- dictions for ultrarelativistic collisions with 16O, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' C 100 (2019) 064912.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='100.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='064912.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='100.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 064912 67.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' N.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Summerfield, B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='-N.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Lu, C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Plumberg, D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Lee, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Noronha-Hostler, A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Timmins, 16O16O collisions at energies available at the bnl relativistic heavy ion collider and at the cern large hadron collider comparing α clustering versus substructure, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' C 104 (2021) L041901.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='104.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='L041901.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='104.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' L041901 68.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Nijs, W.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' van der Schee, Predictions and postdictions for relativistic lead and oxygen collisions with the computational simulation code trajectum, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' C 106 (2022) 044903.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='106.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='044903.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='106.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 044903 15 69.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' W.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Ryssens, G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Giacalone, B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Schenke, C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Shen, Evidence of the hexadecapole deformation of uranium-238 at the relativistic heavy ion collider, in preparation.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 70.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Abdallah, et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=', Tomography of Ultra-relativistic Nuclei with Polarized Photon-gluon Collisions (4 2022).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' arXiv:2204.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='01625.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 71.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' M¨antysaari, B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Schenke, Evidence of strong proton shape fluctuations from incoherent diffrac- tion, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Lett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 117 (2016) 052301.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevLett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='117.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='052301.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevLett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 117.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='052301 72.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Giacalone, B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Schenke, C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Shen, Constrain- ing the nucleon size with relativistic nuclear collisions, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Lett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 128 (2022) 042301.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevLett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='128.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='042301.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevLett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 128.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='042301 73.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' M¨antysaari, B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Schenke, C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Shen, W.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Zhao, Bayesian inference of the fluctuating proton shape, Physics Let- ters B 833 (2022) 137348.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:https://doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1016/ j.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='physletb.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='2022.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='137348.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://www.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='sciencedirect.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='com/science/article/ pii/S0370269322004828 74.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Nijs, W.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' van der Schee, The hadronic nucleus-nucleus cross section and the nucleon size (6 2022).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' arXiv:2206.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 13522.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 75.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Giacalone, There and Sharp Again: The Circle Journey of Nucleons and Energy Deposition (8 2022).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' arXiv:2208.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 06839.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 76.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Everett, et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=', Multisystem bayesian constraints on the transport coefficients of QCD matter, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' C 103 (2021) 054904.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='103.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='054904.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='103.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 054904 77.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' De Vries, C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' De Jager, C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' De Vries, Nuclear charge- density-distribution parameters from elastic electron scat- tering, Atomic Data and Nuclear Data Tables 36 (3) (1987) 495–536.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:https://doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1016/0092-640X(87) 90013-1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://www.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='sciencedirect.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='com/science/article/ pii/0092640X87900131 78.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' P.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' M¨oller, A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Sierk, T.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Ichikawa, H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Sagawa, Nuclear ground-state masses and deformations: FRDM(2012), Atomic Data and Nuclear Data Tables 109-110 (2016) 1–204.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:https://doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1016/j.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='adt.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='2015.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='002.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://www.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='sciencedirect.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='com/science/article/ pii/S0092640X1600005X 79.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Q.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Shou, Y.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Ma, P.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Sorensen, A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Tang, F.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Videbæk, H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Wang, Parameterization of deformed nuclei for Glauber modeling in relativistic heavy ion collisions, Physics Let- ters B 749 (2015) 215–220.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:https://doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1016/ j.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='physletb.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='2015.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='07.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='078.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://www.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='sciencedirect.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='com/science/article/ pii/S0370269315005985 80.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' jie Xu, H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Li, X.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Wang, C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Shen, F.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Wang, Deter- mine the neutron skin type by relativistic isobaric colli- sions, Physics Letters B 819 (2021) 136453.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:https: //doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1016/j.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='physletb.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='2021.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='136453.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://www.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='sciencedirect.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='com/science/article/ pii/S0370269321003932 81.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Jia, C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='-J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Zhang, Scaling approach to nuclear structure in high-energy heavy-ion collisions (11 2021).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' arXiv:2111.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 15559.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 82.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Giacalone, Observing the deformation of nuclei with relativistic nuclear collisions, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Lett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 124 (2020) 202301.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevLett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='124.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='202301.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevLett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 124.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='202301 83.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Giacalone, Constraining the quadrupole deformation of atomic nuclei with relativistic nuclear collisions, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' C 102 (2020) 024901.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='102.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='024901.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='102.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 024901 84.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Jia, S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Huang, C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Zhang, Probing nuclear quadrupole deformation from correlation of elliptic flow and trans- verse momentum in heavy ion collisions, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' C 105 (2022) 014906.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='105.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='014906.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='105.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 014906 85.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' P.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Bo˙zek, Transverse-momentum–flow correlations in relativistic heavy-ion collisions, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' C 93 (2016) 044908.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='93.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='044908.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='93.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 044908 86.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Moreland, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Bernhard, S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Bass, Alternative ansatz to wounded nucleon and binary collision scaling in high-energy nuclear collisions, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' C 92 (2015) 011901.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='92.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='011901.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='92.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 011901 87.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' F.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Gardim, G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Giacalone, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Luzum, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='-Y.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Ollitrault, Effects of initial state fluctuations on the mean trans- verse momentum, Nuclear Physics A 1005 (2021) 121999, the 28th International Conference on Ultra-relativistic Nucleus-Nucleus Collisions: Quark Matter 2019.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi: https://doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1016/j.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='nuclphysa.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='2020.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='121999.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://www.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='sciencedirect.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='com/science/article/ pii/S0375947420303092 88.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Giacalone, F.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Gardim, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Noronha-Hostler, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='-Y.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Ol- litrault, Correlation between mean transverse momentum and anisotropic flow in heavy-ion collisions, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' C 103 (2021) 024909.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='103.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='024909.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='103.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 024909 89.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Aad, et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=', Measurement of flow harmonics correla- tions with mean transverse momentum in lead–lead and proton–lead collisions at √sNN = 5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='02 TeV with the AT- LAS detector, The European Physical Journal C 79 (12) (2019) 985.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1140/epjc/s10052-019-7489-6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1140/epjc/s10052-019-7489-6 90.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Acharya, et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=', Characterizing the initial conditions of heavy-ion collisions at the LHC with mean transverse momentum and anisotropic flow correlations, Physics Let- ters B 834 (2022) 137393.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:https://doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1016/ j.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='physletb.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='2022.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='137393.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://www.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='sciencedirect.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='com/science/article/ pii/S0370269322005275 91.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Jia, Probing triaxial deformation of atomic nuclei in high-energy heavy ion collisions, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' C 105 (4) (2022) 044905.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' arXiv:2109.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='00604, doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 105.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='044905.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 92.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Zhang, An overview of new measurements of flow, chirality, and vorticity from STAR experiment, in: 10th International Conference on New Frontiers in Physics, 2022.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' arXiv:2203.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='13106.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 16 93.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Giacalone, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Jia, C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Zhang, Impact of nuclear deformation on relativistic heavy-ion collisions: Assessing consistency in nuclear physics across en- ergy scales, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Lett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 127 (2021) 242301.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevLett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='127.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='242301.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevLett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 127.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='242301 94.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Sadoudi, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Bender, K.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Bennaceur, D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Davesne, R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Jodon, T.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Duguet, Skyrme pseudo-potential-based EDF parametrization for spuriousity-free MR EDF calculations, Physica Scripta T154 (2013) 014013.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1088/0031-8949/2013/t154/014013.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://doi.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1088%2F0031-8949%2F2013% 2Ft154%2F014013 95.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Borrajo, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' L.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Egido, Symmetry conserving configura- tion mixing description of odd mass nuclei, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' C 98 (2018) 044317.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='98.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='044317.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='98.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 044317 96.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Giacalone, F.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Gardim, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Noronha-Hostler, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='-Y.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Ollitrault, Skewness of mean transverse momentum fluctuations in heavy-ion collisions, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' C 103 (2021) 024910.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='103.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='024910.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' URL https://link.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='aps.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='org/doi/10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content='103.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'} +page_content=' 024910' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/D9E0T4oBgHgl3EQfggHn/content/2301.02420v1.pdf'}